Relationship between the primary and secondary dielectric relaxation processes in propylene glycol and its oligomers

Dielectric relaxation measurements were performed on propylene glycol (PG) and oligomers having different number of repeat units (N=2, 3, and 69). The primary alpha-relaxation had the Kohlrausch-Williams-Watts (KWW) form, wit h a stretch exponent (1-n) which decreased with increasing N. The temperatu re dependence of the alpha-relaxation time, as reflected in the fragility i ndex, increased with N. A broad, rather symmetric secondary beta-relaxation was observed at higher frequencies in the dielectric loss spectrum for all samples with N>1. This is the first observation of the beta-relaxation pea k in dipropylene glycol (N=2) and tripropylene glycol (N=3). The separation between the a-and beta-relaxations increased with increasing N. This trend indicates that the separation is minimal in PG, which makes it difficult t o resolve the beta-relaxation from the more intense alpha-relaxation. This, together with the fact that the strength of the beta-relaxation decreases with the molecular weight of PPG, as found by Johari and coworkers, explain s the absence of an observable beta-peak or shoulder in isothermal or isoch ronal dielectric measurement on PG. It is proposed that the deviation of th e dielectric loss peak for PG from either the KWW or the Cole-Davidson func tions at higher frequencies is due to a beta-relaxation masked by the alpha -process. The same conclusion was reached by Johari and co-workers, based o n evidence from their "difference isochrone method.'' Finally, we show that the data from oligomers of propylene glycol support the recently proposed correlation of tau(beta)(T-g) with (1-n) and the rough agreement between ta u(beta)(T-g) and the primitive relaxation time of the coupling model at tem peratures above T-g. [S0021-9606(99)51423-2].